Figure 5
From: Improving quantum annealing by engineering the coupling to the environment
The probability of being in the ground state at the end of the simulation for a non-complete graph for random \(J_{ij} \sim \mathcal{N}(2,0.1)\). The coupling to the bath is either kept constant or it is optimised. The histograms show the populations of each energy eigenstates at the end of the evolution. Other parameters: \(N=6\), \(\beta = 30\), and \(\omega _{c} = 30\)